Here several useful generator equations are derived.
Often, because maximum power transfer occurrences when impedance is match, there are designs where the generator load equals the internal source resistance. Sure maximum possible power is transferred, but 1/2 of the mechanical input becomes heat inside the generator. Instead, oversize the generator, and use a fraction of the possible power to keep efficiency.
Electrical efficiency as a fraction input mechanical power that is available as electricity a the output terminals. Of course the voltage of the available power might not be optimal - but thats what switching power supplies are for.
Rl = load resistance Rm = motor series (internal) resistance E = Pout / (Pout + Ploss) (efficiency) Pout = I^2 * Rl and Ploss = I^2 * Rm thus E = Rl / (Rl+Rm) let Rl = k * Rm then (define the load resistance as a fraction of the motor series resistance) E = k/(1+k) Thus to keep the efficiency high, then keep the load resistance higher than the motor source resistance, or: Rl >= Rm * E/(1-E) some results: k = 4 -> 80% k = 9 -> 90%
For a load that is a multiple of the generator resistance, a fraction of the maximum possible generator output power is obtained. If the load equals the internal generator resistance, then the maximum output power (Pmax) is obtained (but 1/2 of the input power becomes heat.) Here we can determine the electrical efficiency that results by over sizing the generation
Lets define the power efficiency be: Pe = Pout / Pmax (meaning take Pout from a generate that can supply Pmax) some math... Pe = 4k/(1+k)^2 some more math: let b = 4/Pe - 2; then k = 0.5 * (-b + sqrt(b^2 - 4)) 64% -> k = 4 (80% electrical efficiency) 36% -> k = 9 (90% electrical efficiency) Thus using a generator at 36% of its rated loads results in 90% of the mechanical energy being available as electrical energy.
Its also possible to size a generator based on two fundamental properties of the generator. Here we derive the maximum generator power as a function of rotational velocity omega.
For a generator / motor: omega = Ks * Vemf (Vemf is back emf, and Ks is the speed constant) or Vemf = omega/Ks Vm = Vemf - I * Rm (Vm is voltage at terminals) I = Vm / Rl let Rl = Rm for max output power then Vm = Vemf - (Vm/Rm)*Rm or Vm = omega/Ks - Vm so at max output power Vm = omega/2Ks output power is V^2/R so Pmax = Vm^2 / Rm or Pmax = omega^2 / 4 Rm Ks^2 lets define the power constant as Pk = 1/4RmKs^2 so Pmax = Pk * omega^2
For example: A generator might produce 70 volts at 2500 rpm. The internal resistance is 7.7 ohms. ks = 2500/70 = 35.7 (rpm per volt) Pk = 25e-6 units are v^2/(ohm rpm^2) at 1000 rpm maximum power is 25.5 watts at 2000 rpm 101.8 watts.
A 2nd example is this 490g outrunner motor:
Rs = 0.03, ks = 295 rpm per volt Pk = 1 / 4*0.03*295^2 = 96e-6 at 1000 rpm, max power is 95 watts
3rd example : Himax HC6332-230 Outrunner:
Rs = 0.043, ks = 230 rpm per volt Pk = 109e-6 at 1000 rpm, max power is 109 watts
Powermax EC30-48V :
Rs = .386, ks = 348 Pk = 5.3e-6 at its peak speed of 25,000 rpm - this little motor could produce 3300 watts (and overheat in a few millisconds!) thus this is a great high speed motor to use at fraction of its possible power.